Solar fuels generator

ABSTRACT

The solar fuels generator includes an ionically conductive separator between a gaseous first phase and a second phase. A photoanode uses one or more components of the first phase to generate cations during operation of the solar fuels generator. A cation conduit is positioned provides a pathway along which the cations travel from the photoanode to the separator. The separator conducts the cations. A second solid cation conduit conducts the cations from the separator to a photocathode.

CROSS REFERENCE TO RELATED APPLICATIONS

This Application claims the benefit of U.S. Provisional Patent Application Ser. No. 61/619,316, filed on Apr. 2, 2012, and incorporated herein in its entirety.

STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH

This invention was made with government support under DE-SC000493/T-105066 awarded by the Department of Energy. The government has certain rights in the invention.

FIELD OF THE INVENTION

The invention relates to solar generators, and more particularly, to solar fuels generators.

BACKGROUND

Solar cells are used to generate electrical energy from sunlight. While these cells can generate electricity from sunlight, they do not efficiently store the generated energy. As a result, the energy must be used immediately or stored in devices such as batteries. Storing large amounts of energy in batteries is impractical and expensive. An alternative to storing solar energy in a device is to convert the solar energy into a fuel that can be used at a later time. A solar fuels generator is a device that converts the energy from the sun and water into a fuel such as hydrogen fuel. As a result, there is a need for a practical solar fuels generator.

SUMMARY

The solar fuels generator includes an ionically conductive separator between a first phase and a second phase. The generator also includes an photoanode that uses incident light and one or more components of the first phase to generate cations during operation of the solar fuels generator. The generator also includes a cation conduit that provides a pathway along which the cations travel from the photoanode to the separator.

Another version of the solar fuels generator includes an ionically conductive separator between a first phase and a second phase. The generator also includes a photocathode that uses cations generated from the first phase to generate the solar fuel in the second phase. The generator also includes a cation conduit that provides a pathway along which cations generated at the photoanode can travel from the separator to the photocathode.

A method of generating solar fuels includes generating a cation at a photoanode located in a gaseous first phase. The method also includes conducting the generated cation through a cation conduit to a separator that is located between the first phase and a second phase.

Another method of generating solar fuels includes using cations to generate the solar fuel a photocathode in a gaseous second phase. A separator being between the first phase and the second phase. The method also including conducting the cations through a cation conduit from the separator to a portion of the photocathode that is spaced apart from the separator.

BRIEF DESCRIPTION OF THE FIGURES

FIG. 1 is a cross section of a solar fuels generator.

FIG. 2 is a cross section of another embodiment of a solar fuels generator.

FIG. 3 is a cross section of another embodiment of a solar fuels generator.

FIG. 4 illustrates the solar fuels generator of FIG. 1 included in a system that permits control of delivery of feedstocks to solar fuels generator and removal of the resulting fuel from the solar fuels generator.

FIG. 5 comparers the current density versus applied voltage results for an electrolyzer with liquid water as a feedstock and for a gas with water vapor as the feedstock.

FIG. 6 compares the current density versus applied voltage results for an electrolyzer operating on gas feedstocks with different relative humidity values.

FIG. 7 compares the current density versus applied voltage results for an electrolyzer operating on gas feedstocks with different relative humidity values.

FIG. 8 compares the current density versus applied voltage results for an electrolyzer operating on gas feedstocks with different relative humidity values.

FIG. 9 compares the current density versus applied voltage results for an electrolyzer operating on different carrier gasses.

DESCRIPTION

Prior solar fuels generators use liquid water as the feedstock. One of the difficulties associated with these systems is the generation of gas bubbles such as hydrogen bubbles and oxygen bubbles. The bubbles reduce the contact area between the water and catalysts used by these systems. Further, these bubbles can refract and/or scatter incoming illumination away from the photoelectrodes used in these systems. As a result, the bubbles can reduce the efficiency of the solar fuels generator. This issue can be resolved by switching from a liquid feedstock to a gaseous feedstock. For instance, the feedstock can be a carrier gas that includes water vapor. The water vapor can serve as a reactant in the generation of the solar fuel.

The use of water vapor as a reactant in a solar fuels generator is challenging because of the mass transport issues such as whether enough water can be transported to the electrodes in order to effectively produce a solar fuel. However, the inventors found that with humidified Ar(g) at 20° C. as a feedstock to an electrolyzer, an electrolysis current density of 10 mA cm⁻² was sustained at an applied voltage of 1.6 V and a current density of 20 mA cm⁻² was observed at an applied voltage of ˜1.7 V. Additionally, the inventors surprisingly found that lower voltages were required to support a particular level of current density when using water vapor in the feedstock than were required liquid water was used as the feedstock. Since the voltage that can be achieved by a solar fuels generator that uses light absorption as the voltage source is around 1.5-2 V, these results indicate that that the solar fuels generator can convert water vapor to a solar fuel using terrestrial solar illumination as the energy source. More particularly, these results show that a solar fuels generator can convert water vapor to a hydrogen gas fuel without using an external power source other than unconcentrated light from the sun.

The solar fuels generator includes a separator bewteen a first phase and a second phase. The solar fuels generator also includes one or more photoanodes exposed to the first phase and one or more photocathodes exposed to the second phase. During operation of the solar fuels generator, protons are generated at the photoanodes and then travel through the separator. When the feedstock is a liquid, these protons easily travel from the photoanodes to the separator through the liquid. However, the protons do not readily travel through a gaseous feedstock. As a result, the solar fuels generator employs cation conduits that conduct cations from the photoanodes to the separator. As a result, these cation conduits increase the efficiency of a solar fuels generator using a carrier gas that includes water vapor as the feedstock.

FIG. 1 is a cross section of a solar fuels generator. The solar fuels generator includes a separator that separates a first phase 20 from a second phase 22. Electrodes are positioned in the separator. For instance, photoanodes 12 and photocathodes 14 extend from opposing sides of the separator. Although not shown in FIG. 1, the separator can surround each of the photoanodes 12 and photocathodes 14. The photoanodes and photocathodes convert incident light into excited electron-hole pairs that then drive a chemical reaction The photoanodes 12 include an photoanode light absorber 16 selected to absorb light at a wavelength to which the photoanodes will be exposed during operation of the solar fuels generator. Additionally, the photocathodes include a photocathode light absorber 18 selected to absorb light at a wavelength to which the photocathodes 14 will be exposed during operation of the solar fuels generator.

Suitable materials for the photoanode light absorbers 16 and the photocathode light absorbers 18 include, but are not limited to, semiconductors. In some instances, the photoanode light absorbers 16 include or consist of a semiconductor and/or the photocathode light absorbers 18 include or consist of a semiconductor. The bandgap of the semiconductors included in the photoanode light absorbers 16 can be larger than the bandgap of the semiconductors included in the photocathode light absorbers 18. Suitable semiconductors for the photoanode light absorbers 16 include, but are not limited to, metal oxides, oxynitrides, sulfides, and phosphides that are stable in an oxidizing environment such as WO₃, TiO₂, and TaON. Suitable semiconductors for the photocathode light absorbers 18 include, but are not limited to, p-type silicon, InP, Cu₂O, GaP, and WSe₂.

In some instances, the photoanode light absorbers 16 and/or the photocathode light absorbers 18 are doped. The doping can be done to form one or more pn junctions within the photoanode light absorbers 16 and the photocathode light absorbers 18. For instance, the photoanode light absorber 16 can be an n-type semiconductor while the photocathode light absorber 18 can be a p-type semiconductor. A p-n junction can also be present within either the photocathode light absorbers 18 or the photoanode light absorber 16 or both, and is arranged so that electrons flow from cathode to a reduction catalyst (discussed below) and holes flow from the anode to an oxidation catalyst (discussed below).

The dashed lines at the interface of the photoanode light absorber 16 and the photocathode light absorber 18 illustrate an interface between the materials of the photoanode light absorber 16 and the photocathode light absorber 18. However, the photoanode light absorber 16 and the photocathode light absorber 18 can be the same material and/or include the same dopant. As a result, a photoanode light absorber 16 and the interfaced photocathode light absorber 18 can be a continuous block of material. In these instances, the dashed lines shown in FIG. 1 may represent a feature that is not discernable in the solar fuels generator. One example of a material that can serve as both the photoanode light absorber 16 and the photocathode light absorber 18 is p-type silicon, which can function as the absorber on both the photoanode and photocathode sides of the separator. In particular type silicon is a candidate for the photocathode material because it is cathodically stable under illumination in acidic aqueous media and in conjunction with various metal catalysts can evolve H₂(g) from H₂O.

Other possible choices for the light absorber include semiconductors having wider bandgaps than silicon that are stable in the water vapor medium. Oxide semiconductors are believed to be a possible choice. Some of the light absorbers that can be used as a light absorber include, but are not limited to: tandem structure photoanodes, including tungsten oxide (WO₃), bismuth vanadium oxide (BiVO₄), tantalumoxynitride (TaON), and titanium oxide (TiO₂); tandem structure photocathodes, including silicon (Si), cuprous oxide (Cu₂O), gallium phosphide (GaP), gallium arsenide (GaAs), and indium phosphide (InP); single material electrodes, including strontium titanate (SrTiO₃), strontium niobate (SrNbO₃), and titanium oxide (TiO₂); multijunction photovoltaics, including triple junction amorphous silicon (a-Si), and vertically stacked epitaxially grown III-V semiconductors with tunnel junctions; and series connected photovoltaics, including silicon (Si) cells, gallium arsenide (GaAs) cells, cadmium telluride (CdTe) cells, and Copper Indium Gallium Selenide (CIGS) thin film cells.

The absorption of light by the photocathode light absorber and the photoanode light absorber generates the photovoltage that drive the electrolysis. When semiconductors are used for the photocathode light absorber and the photoanode light absorber, the achievable voltage depends on the choice of semiconductor materials, the associated bandgaps, and doping arrangements as is known in the solar cell arts. Accordingly, the material selections and arrangements can be selected to provide the desired voltage levels. For instance, the tandem and multijunction structures discussed above in which two or more semiconductors in series add their voltages together can be used in order to achieve elevated voltages.

In some instances, the photocathode light absorber 18 and the photoanode light absorber 16 are high aspect ratio structures such as cylinders, wires, or similar shapes with square, rectangular, oval, or irregular cross sections. The aspect ratio is the ratio of the length of the semiconductor: width or diameter of the semiconductor. Narrowing the width of the semiconductors reduces the distance that minority carriers must diffuse radially in order to reach the surface of the semiconductor. Accordingly, a suitable average width for the photocathode light absorbers 18 and/or the photoanode light absorbers 16 can be about the minority-carrier diffusion length of the material. In some instances, the average width for the photocathode light absorbers 18 and/or the photoanode light absorbers 16 is in a range of 100 nm-10 μm.

High aspect ratio structures reduce the charge-carrier flux to the surface of the semiconductor. This reduced flux can reduce the turnover frequency required of any catalysts and can permit the use of more abundant and less active catalysts. Suitable average aspect ratios for the photocathode light absorbers 18 include, but are not limited to, ratios greater than 2:1, or 5:1, and/or less than 50:1, 100:1, or 200:1. Additionally or alternately, suitable average aspect ratios for the photoanode light absorbers 16 include, but are not limited to, ratios greater than 2:1, or 5:1, and/or less than 50:1, 100:1, or 200:1. In one example, the average aspect ratio for the photocathode light absorbers 18 and/or the photoanode light absorbers 16 is in a range of 44:1-70:1. The photoanode light absorbers 16 can have the same average dimensions as the photocathode light absorbers 18 or different average dimensions from the photoanode light absorbers 16. Wire or cylinder shaped photoanode light absorbers 16 and/or the photocathode light absorbers 18 can support the above aspect ratios. The use of high aspect ratio structures is optional.

The separator 10 separates a first phase 20 from a second phase 22. For instance, although not shown, the perimeter of the separator 10 can be clamped between flanges that extend from the side of an enclosure into the interior of the enclosure cell. When the perimeter of the separator 10 is clamped in the flanges, the separator 10 spans the interior of the cell. The first phase 20 can be located in the cell on one side of the separator 10 with the photoanodes 12 in the first phase 20 and the second phase 22 can be located in the cell on the opposing side of the separator 10 with the photocathodes 14 in the second phase 22. The first phase is generally different from the second phase. In some instances, the first phase 20 is a liquid that includes water. In some instances, the first phase 20 is a gas that includes water vapor. The second phase can be a gas or a liquid. In some instances, the first phase 20 is a gas that includes water vapor and the second phase is a gas.

When the first phase is a gas that includes water vapor, a suitable relative humidity for the gas includes relative humidities above 40%, 60% or 70%. Additionally or alternately, when the first phase is a gas that includes water vapor, suitable gas flow rates to each of the photoanodes includes flowrates greater than 0.02 L min⁻¹, or 0.05 L min⁻¹, or 0.2 L min⁻¹. Suitable gasses for use in the first phase include, but are not limited to, Ar, nitrogen, helium, and air. When the second phase is a gas that includes water vapor, in some instances, the second gas has a relative humidity above 40%, 60% or 70%.

The separator 10 is ionically conductive. In some instances, the separator 10 is cationically conductive while concurrently being sufficiently nonconductive to the other components of the first phase and the second phase that the first phase and the second phase remain separated from one another. For instance, in some instances, the separator 10 is cationically conductive and non-conductive or substantially non-conductive to nonionic atoms and/or compounds. In some instances, the separator 10 is cationically conductive while being non-conductive or substantially non-conductive to nonionic atoms and/or nonionic compounds and also to anions. Accordingly, the separator 10 can provide a pathway along which cations can travel from the first phase to the second phase without providing a pathway or a substantial pathway from the first phase to the second phase to one, two, or three entities selected from a group consisting of anions, nonionic atoms or nonionic compounds. In some instances, it may be desirable for the separator 10 to conduct both anions and cations. For instance, when the first phase and/or the second phase has elevated pH levels a separator 10 that conducts both anions and cations may be used. As a result, in some instances, the separator 10 conducts cations and anions but not nonionic atoms or nonionic compounds.

Additionally, the separator should be able to incorporate and support the photoanode light absorbers and the photocathode light absorbers, exchange ions sufficiently to prevent the buildup of a pH gradient, separate the gaseous reaction products sufficiently to prevent them from re-combining, and be sufficiently transparent to the incoming light that the light can be absorbed by both the photoanode light absorbers 16 and the photocathode light absorbers 18; and provide enough structural support to the photoanode light absorbers 16 and the photocathode light absorbers 18 that these structures are sufficiently vertical to provide pathways for the protons to travel to and/or from the separator 10. A suitable separator can be a single layer or material or multiple layers of material. Suitable materials for the separator 10 include, but are not limited to, ionomers and mixtures of ionomers. Ionomers are polymers that include electrically neutral repeating units and ionized repeating units. Suitable ionomers include copolymers of a substituted or unsubstituted alkylene and an acid such as sulfonic acid. In one example, the ionomer is a copolymer of tetrafluoroethylene and perfluoro-3,6-dioxa-4-methyl-7-octene-sulfonic acid. An example is represented by the following Formula I:

wherein m, n, and z are each greater than 0, or each greater than 1. A suitable material having a structure according to Formula I is sold under the trademark NAFION®. NAFION® is an example of a material that is cationically conductive of cations but is not conductive of anions or nonionic atoms or nonionic compounds. Another suitable separator includes NAFION® functionalized with one or more components selected from a group consisting of dimethylpiperazinium cationic groups, glass frits, asbestos fibers, block copolymer formulated layers, and poly(arylene ether sulfone) with quaternary ammonium groups.

The photoanodes 12 include one or more photoanode catalysts 24. The photoanode catalyst can be an oxidation catalyst. When the feedstock includes water vapor, a suitable oxidation catalyst catalyzes water oxidation. The one or more photoanode catalysts 24 can be positioned on the photoanode light absorber 16. In some instances, the one or more catalysts directly contact the photoanode light absorber 16. Additionally or alternately, instances, the one or more photoanode catalysts 24 coat the photoanode light absorber 16 or are positioned in islands on the photoanode light absorber 16. Suitable anode catalysts 24 include, but are not limited to, IrO₂, RuO₂, Co₃O₄, MnO₂, NiFeO_(x) where x is greater than 1 and/or less than 4, IrRuO_(y) where y is greater than 1 and/or less than 4, NiLaO_(z) where z is greater than 1 and/or less than 4, BaSrCoFeO_(z′) where z is greater than 1 and/or less than 4, platinum (Pt), and mixtures thereof. One example of a suitable anode catalyst is a 1:1 IrO₂:RuO₂.

The photocathodes 14 include one or more photocathode catalysts 26. For instance, the photocathode catalyst 26 can be a reduction catalyst that catalyzes the second reaction. For instance, the photocathode catalyst can catalyze proton reduction. The one or more photocathode catalysts 26 can be positioned on the photocathode light absorber 18. In some instances, the one or more catalysts directly contact the photocathode light absorber 18. Additionally or alternately, the one or more photocathode catalysts 26 coat the photocathode light absorber 18 or are positioned in islands on the photocathode light absorber 18 as shown in FIG. 1B. Suitable photocathode catalysts 26 include, but are not limited to, Pt, NiMo, and NiCo.

During operation, the solar fuels generator can be exposed to light such as sunlight, terrestrial solar illumination, AM1 solar radiation, or similar illumination having approximately 1 kilowatt per square meter of incident energy or less. These light sources can be unconcentrated. In some instances, the solar fuels generator is oriented such that the light travels through the photoanodes 12 before reaching the photocathodes 14. Since the photoanode light absorber 16 has a larger bandgap than the photocathode light absorber 18, the photoanodes 12 absorb higher energy (shorter wavelength) light and allow lower energy (longer wavelength) light to pass through the separator 10 to the photocathodes 14. The photocathodes 14 can then absorb the longer wavelengths. Alternately, the light can be incident on both the photoanodes and the photocathodes.

The absorption of light by a photoanode light absorber 16 generates hole-electron pairs within the photoanode light absorber 16. The position of an n-type photoanode light absorber 16 in the first phase 20 produces an electrical field that causes the holes to move to the surface of the photoanode light absorber 16 and then the surface of the photoanode catalyst 24 where the oxidation of the water in the first phase 20 is catalyzed. The oxidation of water is labeled reaction 1 in FIG. 1A. The electrons move from the photoanode light absorber 16 move toward the photocathode light absorber 18 as a result of the electrical field.

The oxidation of the water generates gaseous oxygen and hydrogen cations (H⁺, called protons below). As noted above, the separator 10 is cationically conductive. As a result, the protons can travel through the separator 10 and enter the second phase 22 in response to the pH gradient resulting from the generation of protons in the first phase 20. The movement of the protons from the first phase 20 into the second phase 22 is shown by the arrow labeled A in FIG. 1A.

The absorption of light by the photocathode light absorber 18 generates hole-electron pairs within the photocathode light absorber 18. The presence of a p-type photocathode light absorber 18 in the second phase 22 produces an electrical field that causes the electrons within the photocathode light absorber 18 to move to the surface of the photocathode light absorber 18 and then the surface of the photocathode catalyst 26 where they react with the protons to form hydrogen gas. The reduction of the protons is labeled reaction 2 in FIG. 1. The resulting hydrogen gas can be stored for use as hydrogen fuel. The holes generated in the photocathode light absorber 18 by the absorption of light move from the photocathode light absorber 18 toward the photoanode light absorber 16 as a result of the electrical field and can recombine with the electrons from the photoanode light absorber 16.

Cation conduits 28 are located on the photoanode light absorbers 16 and/or the photocathode light absorbers 18. For instance, the cation conduits 28 are positioned such that a line perpendicular to lateral surfaces of the photoanode light absorbers 16 and/or the photocathode light absorber 18 passes through the cation conduits. In some instances, the cation conduits 28 are located such that the photoanode catalyst 24 is located between the cation conduit 28 and the photoanode light absorber 16 as shown in FIG. 1 and such that a line perpendicular to lateral surfaces of the photoanode light absorbers 16 passes through the photoanode catalyst 24 and also at least one cation conduit 28. When the photoanode catalyst 24 is located between the cation conduit 28 and the photoanode light absorber 16, the cation conduit 28 can be in direct physical contact with the photoanode catalyst 24 or other materials can be located between the cation conduit 28 and the photoanode catalyst 24. Additionally or alternately, the cation conduits 28 can be located such that the photocathode catalyst 26 is located between the cation conduit 28 and the photocathode light absorber 16 and such that a line perpendicular to lateral surfaces of the photocathode light absorbers 18 passes through the photocathode catalyst 26 and also at least one cation conduit 28. When the photocathode catalyst 26 is located between the cation conduit 28 and the photocathode light absorber 18, the cation conduit 28 can be in direct physical contact with the photocathode catalyst 26 or other materials can be located between the cation conduit 28 and the photocathode catalyst 26.

The cation conduits 28 are ionically conductive. In some instances, the cation conduits 28 are cationically conductive while being non-conductive or substantially non-conductive to one, two, or three entities selected from a group consisting of anions, nonionic atoms or nonionic compounds.

The cation conduits 28 can be in direct physical contact with the separator 10. Since the separator 10 and the cation conduits 28 are both cationically conductive, the contact between the cation conduits 28 and the separator 10 provides a pathway that cations can travel from the photoanode 12 side of the separator 10 to the photocathode 14 side of the separator 10. For instance, the arrow labeled B in FIG. 1 shows the movement of the protons from the photoanode 12 side of the separator 10 to the photocathode 14 side of the separator 10. When the first phase is a gas phase, the protons resulting from the first reaction do not readily travel through the first phase to the separator. More particulary, the protons do not readily travel from the photoanode catalyst to the separator through the first pahase. The cation conduits 28 make up for this deficiency by providing an efficient pathway from photoanodes to the separator and then into the second phase. More particulary, when the cation conduits contact the photoanode catalyst and the separator, the cation conduits provide an pathway that the protons can travel from the photoanode catalyst to the separator. As a result, when the first phase is a gas, the dominant pathway that the protons travel from the from the photoanode 12 side of the separator 10 to the photocathode 14 side of the separator 10 may be the pathway indicated by the arrow labeled B rather than the arrow labeled A.

When the second phase is a gas phase, the protons resulting from the first reaction do not readily travel from the separator to the photocathodes through the second phase. More particulary, the protons do not readily travel from the separator to the photocathode catalyst through the second phase. The cation conduits 28 make up for this deficiency by providing an efficient pathway from separator to the photocathodes. More particulary, when the cation conduits contact the photocathode catalyst and the separator, the cation conduits provide a pathway that the protons can travel from separator to the photocathode catalyst.

The cation conduits 28 can include one or more layers or material. The material for the cation conduits 28 on the photoanode side of the separator and the material for the cation conduits 28 on the photocathode side of the separator can be the same or different. In some instances, material for the cation conduits 28 on the photoanode side of the separator and the material for the cation conduits 28 on the photocathode side of the separator are the same material as the separator 10. Further, the cation conduits 28 can be continuous with the separator 10 in that there is not an interface between the cation conduits 28 and the separator 10.

The cation conduits 28 can be a solid or can be included in a layer that is a solid. A suitable material for the cation conduits 28 includes, but is not limited to, ionomers and mixtures of ionomers. Ionomers are polymers that include electrically neutral repeating units and ionized repeating units. Suitable ionomers include copolymers of a substituted or unsubstituted alkylene and an acid such as sulfonic acid. In one example, the ionomer is a copolymer of tetrafluoroethylene and perfluoro-3,6-dioxa-4-methyl-7-octene-sulfonic acid. An example is represented by the following Formula I:

wherein m, n, and z are each greater than 0, or each greater than 1. A suitable material having a structure according to Formula I is sold under the trademark NAFION®.

As noted above, the cation conduits 28 and the separator 10 can be constructed of the same material and can optionally be continuous with the separator 10. However, even when cation conduits 28 and the separator are constructed of the same material, the cation conduits 28 and the separator 10 can have a different thickness. In some instances, all or a portion of the cation conduits 28 are thin enough that a reactant can diffuse through the cation conduit 28 to the underlying catalyst. For instance, the cation conduits 28 on the photoanode side of the separator can be thin enough to permit the water from water vapor or liquid water to diffuse through the cation conduit 28 to the underlying catalyst. This diffusion of water through the cation conduit 28 allows the first reaction shown in FIG. 1 to occur at a surface of the photoanode catalyst 24. In contrast, the separator 10 can be thick enough to support the photoanode light absorbers and/or the photocathode light absorbers such that the far end of each light absorber is held above the separator 10. Increasing the portion of the light absorber embedded in the separator 10 can increase the support of the light absorber. However, it is possible that increasing the portion of the semiconductor in the separator 10 can increase the portion of light that is absorbed by the separator 10 rather than by the light absorbers. A suitable average percentage of the photoanode light absorber length and/or photocathode light absorber length that is inside of the separator 10 includes percentages greater than 5%, or 20% and/or less than 80%, or 100%. As a result, the separator may be thicker than the cation conduits 28. For instance, a ratio for a thickness of the separator to a thickness of one or more of the cation conduits can be greater than 5:1, 50:1, or 100:1.

Although FIG. 1 illustrates the cation conduits 28 extending from the separator and then up the entire length of the photoanode light absorbers 16 and the photocathode light absorbers 18, the cation conduits 28 can extend only part way up the length of the photoanode light absorbers 16 and/or the photocathode light absorbers 18. For instance, the cation conduits 28 can extend more than 10%, 30% or 50% and/or less 70% or 90% up the length of the photoanode light absorbers 16 and/or the photocathode light absorbers 18.

Although the solar fuels generators of FIG. 1 illustrate the cation conduits 28 as a layer of material over a layer of the photoanode catalyst 24 or the photocathode catalyst 26, the layer represented by the photoanode catalyst 24 or the combination of layers represented by the photoanode catalyst 24 and the touching cation conduit 28 can be a layer where the photoanode catalyst 24 is dispersed through the cation conduit 28. As an example, the layer represented by the photoanode catalyst 24 can be a layer where the photoanode catalyst or particles of the photoanode catalyst are coated with the cation conduit 28. Additionally or alternately, the layer represented by the photocathode catalyst 26 or the combination of layers represented by the photocathode catalyst 26 and touching conduit 28 can be a layer where the photocathode catalyst 26 is dispersed through the cation conduit 28. As an example, the layer represented by the photocathode catalyst 26 can be a layer where the photocathode catalyst 26 or particles of the photocathode catalyst 26 are coated with the cation conduit 28. In these arrangements, the cation conduit 28 provides a pathway along which the cations can travel through the photocathode catalyst 26 and also through the photoanode catalyst. For instance, the line labeled B can illustrate the path of the protons from the first phase to the second phase. As a result, these embodiments of the solar fuels generator can operate as disclosed in the context of FIG. 1.

The components of FIG. 1 can be re-arranged to achieve other solar fuels generators as shown in FIG. 2 and FIG. 3. The solar fuels generators of FIG. 1 through and FIG. 3 illustrate the cation conduits 28 as a layer of material over a layer of the photoanode catalyst 24 or the photocathode catalyst 26. However, the layer represented by the photoanode catalyst 24 or the combination of layers represented by the photoanode catalyst 24 and the touching cation conduit 28 can be a single layer where the photoanode catalyst 24 is dispersed through the cation conduit 28. As an example, the layer represented by the photoanode catalyst 24 or the layers represented by the photoanode catalyst 24 and the touching cation conduit 28 can be a single layer where the photoanode catalyst or particles of the photoanode catalyst are coated with the cation conduit 28. Further, the layer represented by the photocathode catalyst 26 or the combination of layers represented by the photocathode catalyst 26 and touching conduit 28 can be combined into a single layer where the photocathode catalyst 26 is dispersed through the cation conduit 28. As an example, the layer represented by the photocathode catalyst 26 or the layers represented by the photocathode catalyst 26 and the touching cation conduit 28 can be a single layer where the photocathode catalyst 26 or particles of the photocathode catalyst 26 are coated with the cation conduit 28. In the solar fuels generators of FIG. 2 and FIG. 3, when these material arrangements are used, the presence of cation conduit 28 in the layer of photoanode catalyst and/or in the layer of photoanode catalyst provides a pathway along which the cations can travel through the photocathode catalyst 26 and also through the photoanode catalyst 24. For instance, the line labeled B in FIG. 2 and FIG. 3 can illustrate the path of the protons from the first phase to the second phase. As a result, these embodiments of the solar fuels generator can operate as disclosed in the context of FIG. 1. A suitable method for coating a catalyst with a cation conductor includes, but is not limited to, casting the catalyst in a liquid solution containing the ionomer and later processing that ionomer to an active membrane form.

The photoanode catalyst 24 and/or photocathode catalyst 26 can include materials in addition to the catalyst. For instance, the above layers that includes photoanode catalyst 24, layers that include photoanode catalyst 24 and cation conduit 28, layers that includes a photocathode catalyst 26, and layers that include photocathode catalyst 26 and cation conduit 28 can include one or more components selected from a group consisting of electrically conductive fillers, electrically conductive materials, diluents, and/or binders. For instance, a layer can include a metal mesh or metal substrate that provides support to the catalyst and/or cation conduit and/or enhances the electrical conductivity of the catalyst and/or cation conduit. In some instances, the metal mesh or substrate acts as a current collector. A suitable method for forming a layer that includes an electrically conducting mesh or substrate, a catalyst and optionally a cation conduit includes hot pressing a mesh to a membrane and casting catalyst particles on the metal mesh from a solution of the membrane ionomer material.

The above illustrations show that the light absorbers in direct contact with the catalysts in order to provide electrical communication between the light absorbers and catalysts. However, this electrical communication can be achieved through other mechanisms. For instance, a metal mesh or metal substrate in a catalyst layer can be connected directly to the appropriate light absorber or an electrical conductor such as a metal trace or wire can be used to connect the metal mesh or substrate in a catalyst layer to the appropriate light absorber.

FIG. 4 illustrates the solar fuels generator of FIG. 1 included in a system that permits control of delivery of feedstocks to the photoanodes and removal of the fuel from the photocathodes. Although the system of FIG. 4 includes the solar fuels generator of FIG. 1, the illustrated system can be used in conjunction with the other solar fuels generators disclosed above.

The solar fuels generator is positioned in an enclosure 29 such that the solar fuels generator separates the first phase and the second phase. All or a portion of the enclosure 29 can be fully or partially transparent to the light that is to be incident on the electrodes. The enclosure 29 defines a first chamber 30 having an inlet port 32 and an outlet port 34. The feedstock can enter the first chamber 30 through the inlet port 32 and the resulting contents of the first chamber 30 can exit the first chamber 30 through the outlet port 34. In the case where the feedstock is a gas that includes water vapor, the gas can enter the first chamber 30 through the inlet port 32 and exit the chamber through the outlet port 34. As a result, the inlet port 32 and the outlet port 34 can be used to control the content and characteristics of the first phase.

The enclosure 29 can also define a second chamber 36 having an inlet port 38 that optionally includes an inlet valve 40 and an outlet port 42 that optionally includes an outlet valve 44. A gaseous or liquid supply stream can enter the second chamber 36 through inlet port 38 and the resulting second phase can exit the second chamber 36 through the outlet port 42. As a result, the inlet port 38 and the outlet port 34 can be used to control the content and characteristics of the second phase. For instance, the second chamber 36 can be filled and maintained in a close state by closing the two valves on the second inlet port 38 and the second outlet port 42 so that a reaction can be run in a batch mode. Alternatively, the valves can be maintained in an open condition or removed from the system so that a reaction can be run in a continuous mode.

The reaction that takes place on the photocathode side of the separator can be supported entirely by the flux of protons (H⁺) that flow across the separator, and no net provision of protons on the photocathode side from another source is needed but can optionally be provided. While no source of hydrogen needs to be provided, it may be advantageous to have a source of water or water vapor on the photocathode side of the separator. For instance, the supply stream and second phase can include water or water vapor. The presence of water or water vapor in the supply stream can help to hydrate the separator. Separators such as NAFION® should be hydrated in order to maintain high ionic conductivity because water preferentially fills hydrophilic, negatively charged channels enable the selective transfer of protons across the separator. Without sufficient water present, the channels constrict and the separator conductivity is significantly reduced. In addition or as an alternative to including water or water vapor in the supply stream, hydration of the separator may be possible by periodically or continually sprinkling or misting the separator with water. Alternatively, a NAFION® separator could be fabricated with a web of hydroponic polymer integrated into the separator that would wick water from a reservoir located in the system. In some instances, separator materials that are less sensitive to water content are used.

In addition or as an alternative to water and/or water vapor. The supply stream and second phase can include a carrier gas. The carrier can be selected to carry away the generated fuel to a collection location. Additionally or alternately, the carrier gas can be used to maintain a target pressure within the second chamber 36. In some instances, a suitable pressure is in the approximate range of 1 atmosphere or ambient pressure. A suitable carrier gas for inclusion in the second phase includes, but is not limited to, Ar, Ntirogen and CO₂.

The supply stream and/or the second phase can also include or consist of a reactant. Although the above discussion discloses using the solar fuels generator to generate hydrogen gas for use as a fuel, the solar fuels generator can be employed to generate other fuels that include hydrocarbons such as methane. Hydrocarbon fuels include or consists of carbon and hydrogen and may include or consist of carbon, hydrogen, and oxygen. These fuels can be generated by delivering an additional reactant to the photocathodes. For instance, the supply stream and/or second phase can include one or more additional reactants. The following generalized reaction can represent the overall reaction used by the solar fuels generator in the generation of these fuels:

M CO₂+N H₂O→C_(M)H₂NO_((2M+N−2P))+P O₂   (Equation 1)

where M, N, and P are non-negative numbers and, in some instances, are integers. C_(M)H₂NO_((2M+N−2P)) represents the fuel produced in this reaction and CO₂ serves as the reactant that is delivered to the photocathodes. Examples of the fuels that can be produced using this reaction in combination with the disclosed solar fuels generator include carbon monoxide, methanol, methane, ethanol, and formic acid. The following table 1 presents values for M, N and P that can be used to generate a particular fuel.

TABLE 1 M N P Fuel Chemical Name 1 2 2 CH₄ Methane 2 4 3 2 molecules of CH₃OH Methanol produced 2 2 1 2 molecules of HCOOH Formic acid produced 2 2 2 CH₃COOH Acetic Acid 2 3 3 C₂H₆O Ethanol 3 3 4 CH₃CH₂COH Propanol 3 4 4 HOCH₂CH₂CH₂OH 1,3-Propanediol 4 3 4 CH₃CH₂COCOOH 2-Oxybutyric acid 4 5 6 CH₃CH₂CH₂COH Butanol 6 6 6 C₆H₁₂O₆ Glucose

The half reactions for each of the above fuels illustrate how the solar fuels cell generates a particular one of the hydrocarbon fuels in the above Table 1. For instance, when using the solar fuels cell to generate methanol, the half reaction at the photoanode, the half reaction at the photocathode and the overall reaction are as follows:

$\frac{\begin{matrix} {3\left( {H_{2}{O(g)}}\rightarrow{{O_{2}(g)} + {4H^{+}} + {4\; e^{-}}} \right)\left( {{reaction}\mspace{14mu} {at}\mspace{14mu} {the}\mspace{14mu} {photoanode}} \right)} \\ {2\left( {{CO}_{2} + {6\; H^{+}} + {6\; e^{-}}}\rightarrow{{{CH}_{3}{OH}} + {H_{2}O}} \right)\left( {{reaction}\mspace{14mu} {at}\mspace{14mu} {the}\mspace{14mu} {photocathode}} \right)} \end{matrix}}{\left. {{4\; H_{2}O} + {2\; {CO}_{2}}}\rightarrow{{2\; {CH}_{3}{OH}} + {3\; {{O_{2}\left( {{overall}\mspace{14mu} {reaction}} \right)}.}}} \right.}$

Since the overall reaction is Equation 1 with M=N=P=6, these half reactions show the relationship between the overall reaction and the half reactions at the photoanodes and the photocathodes. Additionally, the reaction at the photoanode is the same as the first reaction disclosed in FIG. 1. The protons and electrons are provided to the photocathode as a result of the reaction at the photoanode followed by flow of the protons and electrons across the separator. As a result, the primary chemical change needed to generate methanol instead of hydrogen is the delivery of the CO₂ to the photocathode as a reactant.

As is evident from Equation 1, each of the hydrocarbon fuels generated through the use of Equation 1 is generated by delivering CO₂ to the photocathodes as a reactant. It is believed that a particular one of the hydrocarbon fuels can be generated by controlling variables such as the proportions (or partial pressures) of the reactant, the temperature of the reaction, the voltages applied to the catalysts, and the chemical composition of the catalysts. The Equiation 1 reaction that produces glucose represents photosynthesis. Photosynthesis occurs at ambient temperatures in the vicinity of room temperature (e.g., in the range of 10 to 40° C., and possibly in the range of 0 to 100° C.). As a result, it is believed that operating the solar fuels generator at temperatures in these ranges can generate glucose.

When the second phase includes a reactant, the photocathode catalyst can be altered to catalyze the reaction at the photocathode. For instance, when the second phase includes CO₂ as a reactant, a suitable photocathode catalyst 26 can include one or more components selected from the group consisting of copper (Cu), zinc (Zn), tin (Sn), nickel (Ni), platinum (Pt), palladium (Pd), rhodium (Rh), iridium (Ir), metal porphyrins and phthalocyanines. Other metals can also serve as a photocathode catalyst 26 when the second phase includes CO₂ as a reactant.

Although the enclosure 29 is disclosed as defining two chambers, a suitable enclosure 29 may be configured to define a single chamber in which the photoanodes are positioned or in which the photocathodes are positioned. In some instances, the enclosure 29 includes heating elements in order to permit the solar fuels generator to operate at higher temperatures. The heating elements can be active heating elements that require an external energy source such as resistive heaters, heated fluid heaters, or combustion based heaters. Additionally or alternately, the heating elements can be passive heating elements where an external energy source is not required. For instance, the heating elements can be a black body layer that produces heat by collecting light not absorbed by the photoanode light absorbers or the photocathode light absorbers. Additionally or alternately, elevated temperatures may be achieved by heating the supply stream and/or the feedstock. Elevated temperatures may be able to provide higher current densities. Further, higher temperature gasses can have a greater water content that can further increase the current density. Additionally, the use of elevated temperatures may aid in generating particular hydrocarbons. Since the following experimental results establish that hydrolization of water can be achieved using only solar illumination at atmospheric conditions as the only energy source for the solar fuels generator, in some instances, the system excludes active heating elements and/or passive heating elements.

A suitable method of forming the separator on the anode light absorbers and the cathode light absorbers includes, but is not limited to, solution casting an ionomer material onto the semiconductor. A suitable method for applying an anode catalyst to the anode light absorbers includes, but is not limited to, electrodeposition, sputtering, electroless deposition, spray pyrolysis, atomic layer deposition, etc. A suitable method for applying a cathode catalyst to the anode light absorbers includes, but is not limited to, electrodeposition, sputtering, electroless deposition, spray pyrolysis, atomic layer deposition, etc. A suitable method for forming the cation conduit on the cathode catalyst and/or the anode catalyst includes, but is not limited to, solution casting the ionomer material onto the semiconductor and/or catalyst.

EXAMPLES Example 1

An electrolyzer was used to explore the performance of the solar fuels generator with water vapor as the feedstock. The electrolyzer components were obtained from Clean Fuel Cell Energy, LLC, 3350 Ulmerton Road, Suite 23, Clearwater, Fla. 33762). In contrast to the solar fuels generators disclosed above, the electrolyzer used an external power source to generate the electrolysis voltage. The electrolyzer included two graphite end plates (one for the photoanode and one for the photocathode) that had serpentine gas flow channels (1.8 mm wide, 2.0 mm deep, spaced 1.0 mm apart) grooved into the side of the plate that faced the separator. The channels represented ˜80% of the active area of the separator that was directly exposed to the input gas flow. In other embodiments, a serpentine pattern having narrower channels and closer spacing may be advantageous to better match the electrical characteristics of the catalysts (such as charge carrier diffusion lengths) and the mechanical spacing of the graphite contacts to the catalysts. The separator was NAFION® (available from Lynntech Inc., 2501 Earl Rudder Freeway South, Suite 100, College Station, Tex. 77845, NAFION® 115, 127 μm thick) that had a photoanode catalyst loading of 3.0 mg cm⁻² of IrRuO_(x) (1:1IrO2:RuO2) and a photocathode catalyst loading of 3.0 mg cm⁻² of Pt black. The projected active area of the separator was 5 cm². Gas diffusion layers were not used, due to the instability under electrolysis conditions of the carbon-based material in a typical gas diffusion layer.

Ultra-high purity Argon gas (UHP Ar(g)) (>99.99%) was used as the carrier gas in all experiments, except for those specifically identified experiments in which the carrier gas was either N₂(g) (>99.99%) or house air (1.10±0.15 ppth of water vapor). The carrier gas was saturated with water vapor by passing the gas at a flow rate of 0.04-0.5 L min-1 (controlled by flowmeters from Chemglass) through a bubbler that had been filled with 18 MΩ-cm resistivity deionized H₂O, obtained from a Barnstead Nanopure system. The humidified gas stream was mixed with a dry gas stream, both at controlled flow rates, to create a gas flow of the desired relative humidity (RH). The system produced precise (±2% RH) and reproducible humidity values in the gas flow stream, as monitored by a relative humidity probe (Omega, RH-USB sensor). A water-saturated carrier gas stream to which dry gas had not been added had a RH of ˜95%. To minimize the back diffusion of ambient oxygen into the electrolysis unit, the output stream from the electrolyzer was bubbled through an oil bath. For the electrolysis of liquid water, the electrolyzer cell was immersed in 18 MΩ-cm resistivity H₂O (1) that had been deoxygenated by bubbling with Ar(g) for >1 h. All experiments were conducted at an ambient temperature of 20° C.

The electrolyzer was allowed to equilibrate at open circuit for more than 2 h before measurements of the current density-voltage (J-V) behavior under each set of experimental conditions (flow rate, RH, etc.) were performed. An SI model 1286 Schlumberger Potentiostat was used to apply a DC bias to the electrolyzer cell, and to measure the current through the cell, through current collector pins in contact with each of the graphite end plates of the electrolysis unit. The current reached an approximate steady state value after more than 300 s at each applied bias. The J-V behavior was also measured by sweeping the voltage, at a scan rate of 1 mV s⁻¹, from open circuit to 2.6 V. The current values measured at a given potential in the scan were in close agreement with the current that was measured at that same potential after 300 s under potentiostatic conditions. The current density was determined using the projected area of the active part of the separator electrode assembly without correcting for the estimated area in direct contact with the graphite end plates of the electrolyzer. In an electrolyzer for use in a system having no electrical connection to an external power source, a photoabsorber such as a photovoltaic cell or photovoltaic array can be used to provide the potential between the photocathode and the photoanode, to provide the needed charge carriers.

The current density versus applied voltage (J-V) results are presented in FIG. 5 for the electrolyzer with liquid water as a feedstock and for the Ar(g) saturated with water vapor as the feedstock. The information provided in the legend specifies the gas flow rate to the photoanode/photocathode. The carrier gas was UHP Ar(g) with a RH of 95% in each case, and the operating temperature was 20° C. The data represented by diamonds is the J-V behavior of the electrolyzer immersed in liquid water at 20° C. For J<30 mA cm⁻², the J-V results were very similar for both the liquid feedstock and the water vapor feedstock. At a given voltage, more current was observed with water vapor as the feedstock than with liquid water as the feedstock. The limiting electrolysis current density increased with increasing Ar(g)/H₂O(g) flow rate, from a value of ˜25 mA cm⁻² at 0.05 L min⁻¹ to ˜40 mA cm⁻² at a flow rate of 0.3 L min⁻¹ to each electrode. In contrast, when immersed in liquid water, the electrolyzer did not reach a limiting current density within the experimentally measured voltage range.

Since a solar fuels generator constructed as disclosed above can provide a voltage of around 1.5-2.0 V depending on the structure and materials used in the photoanode light absorber and the photocathode light absorber, the results show that electrolysis in a solar illuminated solar fuels generator can sustained electrolysis at a current density of J=10-20 mA cm⁻² with water vapor as the feedstock. Further, the flux of water molecules to the separator limited the current density at higher current densities. However, higher flow rates of humidified gas to the electrolyzer can provide an increased mass flux of water to the separator surface, reducing the effect of mass transport limitations. For instance, increasing the flow rate of humidified Ar(g) to each electrode, from 0.05 L min⁻¹ to 0.3 L min⁻¹, increased the limiting electrolysis current density by 60% (from 25 mA cm⁻² to 40 mA cm⁻²). These results are lower bounds on the attainable current density in such a system because no gas diffusion layer was used and the graphite end plates were directly attached to the catalyst layer, so only the portion (˜80%) of the catalyst that was directly exposed to the gases, and then only the fraction that was within useful electrical contact laterally to the electrodes, was electrochemically active as configured in this test system.

Example 2

Current density versus applied voltage (J-V) results are presented in FIG. 6 for the electrolyzer using Ar(g) carrier gas with water vapor as the feedstock. The relative humidity of the input carrier gas was varied. The information provided in the legend specifies the relative humidity of the gas stream to the photoanode/photocathode. As is evident from the legend, this data was generated for equal levels of relative humidity on both sides of the separator. In each case, the carrier gas was UHP Ar(g) at a flow rate of 0.2 L min⁻¹ in each case, and the operating temperature was 20° C.

These results show that decreases in relative humidity can reduce electrolysis performance. The data also shows that very low levels of electrolysis current sustained at a relative humidity of ≦60%. Without being bound to theory, it is believed that the drop in the electrolysis performance may be due to drying of the separator.

Example 3

Current density versus applied voltage (J-V) results are presented in FIG. 7 for the electrolyzer using Ar(g) carrier gas with water vapor as the feedstock. The relative humidity of the input carrier gas was varied in the second phase but not in the first phase. The information provided in the legend of FIG. 7 specifies the relative humidity of the gas stream to the photoanode/photocathode.

Current density versus applied voltage (J-V) results are presented in FIG. 8 for the electrolyzer using Ar(g) carrier gas with water vapor as the feedstock. The relative humidity of the input carrier gas was varied in the first phase but not in the second phase. The information provided in the legend of FIG. 8 specifies the relative humidity of the gas stream to the photoanode/photocathode.

The difference between the J-V behavior when reducing humidity at the photocathode (FIG. 7) and reducing humidity at the photoanode (FIG. 8) was fairly minor, the electrolyzer performed somewhat better when the relative humidity was reduced at the photocathode. This result may occur because water is decomposed at the photoanode and accordingly lowers the water content at the photoanode as compared to the photocathode.

Example 4

Current density versus applied voltage (J-V) results are presented in FIG. 9 for the electrolyzer when varying different carrier gasses in the first phase and the second phase. For instance, the carrier gas was varied between Argon gas (UHP Ar(g)) (>99.99%), N₂(g) (>99.99%) or house air (1.10±0.15 ppth of water vapor). The legend specifies the carrier gas delivered to the photoanode/photocathode. The addition of O₂(g) in air to the carrier gas feed to the photoanode appears to have little effect on the behavior of the electrolyzer. However, the presence of O₂(g) in air at the photocathode had a strong effect on the J-V behavior of the electrolyzer.

These results indicate that when O₂(g) in air is delivered to the photocathode, the photocathode is essentially performing the opposite reaction to the photoanode, reducing O₂(g) back into water by combining O₂(g) with protons coming from the separator. The onset of current occurred for V greater than 500 mV, rather than at 0 V, due to the catalytic overpotential. Because the reduction of O₂(g) is thermodynamically favored relative to H₂(g) evolution, the steady-state flux of O₂(g) to the catalyst sites at the photocathode impairing overall cell efficiency. The results also indicate that above 1.5 V, H₂(g) evolution occurs at the photocathode and competes kinetically with O₂(g) reduction in consuming protons. If H₂(g) is produced rapidly enough relative to the input air flow rate, the H₂(g) could purge the O₂(g) from the catalyst surface, ensuring maximum H₂(g) production. The H₂(g) will need to be separated from any O₂(g) in the photocathode effluent downstream before the gases recombine to form water. If no O₂(g) is input to the photocathode, the photocathode should self-purge and become depleted of O₂(g), except for the steady-state O₂(g) crossover from the photoanode. Therefore, while it is possible to expose the photoanode of a water vapor photoelectrolysis system to the atmosphere during operation in the field, the introduction of air to the photocathode is desirable under conditions for which the reduction of O₂(g) is not replacing the evolution of H₂(g).

Although the solar fuels generator is disclosed as being used in combination with a gaseous first phase and a gaseous second phase, the first phase and/or the second phase can be a fluid, liquid, or solid.

Other embodiments, combinations and modifications of this invention will occur readily to those of ordinary skill in the art in view of these teachings. Therefore, this invention is to be limited only by the following claims, which include all such embodiments and modifications when viewed in conjunction with the above specification and accompanying drawings. 

1. A solar fuels generator, comprising: an ionically conductive separator between a first phase and a second phase; a photoanode that uses one or more components of the first phase to generate cations during operation of the solar fuels generator; and a cation conduit positioned so as to provide a pathway along which the cations travel from the photoanode to the separator.
 2. The generator of claim 1, wherein the photoanode includes an oxidation catalyst.
 3. The generator of claim 1, wherein the pathway extends from the oxidation catalyst to the separator.
 4. The generator of claim 1, wherein: the photoanode extends outward from a first side of a separator; and a photocathode extends outward from a second side of the separator, the second side being opposite from the first side.
 5. The generator of claim 1, wherein the cation conduit is in direct physical contact with the separator.
 6. The generator of claim 1, wherein the photoanode includes an oxidation catalyst between the cation conduit and a side of the photoanode.
 7. The generator of claim 1, wherein the cation conduit is in direct physical contact with the separator and extends outward from the separator along a side of the photoanode.
 8. The generator of claim 1, wherein the photoanode is one of a plurality of photoanodes that each uses one or more components of the first phase to generate cations during operation of the solar fuels generator.
 9. The generator of claim 1, wherein the cation conduit is the same material as the separator.
 10. The generator of claim 1, wherein the cation conduit is the same material as the separator and the cation conduit is continuous with the separator.
 11. The generator of claim 1, wherein the first phase is a gas that includes water vapor, the second phase is a gas, and the photoanode is configured to use the water vapor to generate the cations.
 12. The generator of claim 1, wherein the cation conduit includes a copolymer of a substituted or unsubstituted alkylene and an acid.
 13. The generator of claim 12, wherein the acid is a sulfonic acid.
 14. The generator of claim 1, wherein the separator conducts the cations.
 15. The generator of claim 1, wherein the pathway extends from the separator to a portion of the photoanode that is distant from the separator.
 16. The generator of claim 1, further comprising: a photocathode generates the solar fuel in the second phase, and a second cation conduit positioned so as to conduct cations conducted through the separator from the separator to a portion of the photocathode that is spaced apart from the separator.
 17. The generator of claim 16, wherein the photocathode includes a reduction catalyst between the second cation conduit and a side of the photocathode.
 18. The generator of claim 16, wherein the second cation conduit is in direct physical contact with the separator and extends outward from the separator along the lateral side of the photocathode.
 19. A solar fuels generator, comprising: an ionically conductive separator between a first phase and a second phase; a photocathode that uses cations generated from the first phase to generate the solar fuel in the second phase; and a cation conduit positioned so as to provide a pathway along which cations generated at the photoanode can travel from the separator to the photocathode.
 20. A method of generating solar fuels, comprising: generating a cation at a photoanode in a gaseous first phase; and conducting the generated cation through a cation conduit to an ionically conducting separator located between the first phase and a second phase. 